对“光子尖峰神经元激子-极化子凝聚体的漏-积-燃机制”的修正

IF 9.8 1区物理与天体物理 Q1 OPTICS

Laser & Photonics Reviews Pub Date : 2024-12-05 DOI:10.1002/lpor.202401760

{"title":"对“光子尖峰神经元激子-极化子凝聚体的漏-积-燃机制”的修正","authors":"","doi":"10.1002/lpor.202401760","DOIUrl":null,"url":null,"abstract":"K. Tyszka, M. Furman, R. Mirek, M. Król, A. Opala, B. Seredyński, J. Suffczyński, W. Pacuski, M. Matuszewski, J. Szczytko, B. Piętka, Leaky Integrate-and-Fire Mechanism in Exciton–Polariton Condensates for Photonic Spiking Neurons. Laser Photonics Rev 2022, 17, 2100660. https://doi.org/10.1002/lpor.202100660In this article, an error was identified in the caption and panel numbering of Figure 5. Panels (d) and (e) were inadvertently switched, and two of the panel references were omitted from the caption.The revised version of Figure 5, along with its caption, is provided below.Figure 5 (a) Dependence of the delay <math>\n <semantics>\n <mrow>\n <mi>Δ</mi>\n <mi>t</mi>\n </mrow>\n <annotation>$\\Delta {\\mathrm{t}}$</annotation>\n </semantics></math> between the peak of the pumping pulse P(t) and the peak of the condensate emission <math>\n <semantics>\n <mrow>\n <msub>\n <mi>n</mi>\n <mi>C</mi>\n </msub>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation>${{{\\mathrm{n}}}_{\\mathrm{C}}}( {\\mathrm{t}} )$</annotation>\n </semantics></math> on the peak pumping power P. (b, c) Evolution of condensate density <math>\n <semantics>\n <mrow>\n <msub>\n <mi>n</mi>\n <mi>C</mi>\n </msub>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation>${{{\\mathrm{n}}}_{\\mathrm{C}}}( {\\mathrm{t}} )$</annotation>\n </semantics></math> and the inactive reservoir density <math>\n <semantics>\n <mrow>\n <msub>\n <mi>n</mi>\n <mi>i</mi>\n </msub>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation>${{{\\mathrm{n}}}_{\\mathrm{i}}}( {\\mathrm{t}} )$</annotation>\n </semantics></math> for the two pumping powers marked in (a). (d, e) The corresponding evolution of the active reservoir density <math>\n <semantics>\n <mrow>\n <msub>\n <mi>n</mi>\n <mi>R</mi>\n </msub>\n <mrow>\n <mo>(</mo>\n <mi>t</mi>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation>${{{\\mathrm{n}}}_{\\mathrm{R}}}( {\\mathrm{t}} )$</annotation>\n </semantics></math>. Parameters: <math>\n <semantics>\n <mrow>\n <msub>\n <mi>γ</mi>\n <mi>C</mi>\n </msub>\n <mo>=</mo>\n <mn>1</mn>\n <mo>/</mo>\n <mn>12</mn>\n </mrow>\n <annotation>${{{{\\gamma}}}_{\\mathrm{C}}} = 1/12$</annotation>\n </semantics></math> (1/ps), <math>\n <semantics>\n <mrow>\n <msub>\n <mi>γ</mi>\n <mi>R</mi>\n </msub>\n <mo>=</mo>\n <mn>1</mn>\n <mo>/</mo>\n <mn>200</mn>\n </mrow>\n <annotation>${{{{\\gamma}}}_{\\mathrm{R}}} = 1/200$</annotation>\n </semantics></math> (1/ps), <math>\n <semantics>\n <mrow>\n <msub>\n <mi>γ</mi>\n <mi>I</mi>\n </msub>\n <mo>=</mo>\n <mn>1</mn>\n <mo>/</mo>\n <mn>1000</mn>\n </mrow>\n <annotation>${{{{\\gamma}}}_{\\mathrm{I}}} = 1/1000$</annotation>\n </semantics></math> (1/ps), <math>\n <semantics>\n <mrow>\n <mi>R</mi>\n <mo>=</mo>\n <mn>6</mn>\n <mo>×</mo>\n <msup>\n <mn>10</mn>\n <mrow>\n <mo>−</mo>\n <mn>4</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>${\\mathrm{R}} = 6 \\times {{10}^{ - 4}}$</annotation>\n </semantics></math>(<math>\n <semantics>\n <mrow>\n <mi>μ</mi>\n <msup>\n <mi>m</mi>\n <mrow>\n <mn>2</mn>\n <mspace></mspace>\n </mrow>\n </msup>\n </mrow>\n <annotation>${{\\umu}}{{{\\mathrm{m}}}^{2\\ }}$</annotation>\n </semantics></math>/ps), <math>\n <semantics>\n <mrow>\n <mi>κ</mi>\n <mo>=</mo>\n <mn>5</mn>\n <mo>×</mo>\n <msup>\n <mn>10</mn>\n <mrow>\n <mo>−</mo>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>${{\\kappa}} = 5 \\times {{10}^{ - 2}}$</annotation>\n </semantics></math>(<math>\n <semantics>\n <mrow>\n <mi>μ</mi>\n <msup>\n <mi>m</mi>\n <mrow>\n <mn>2</mn>\n <mspace></mspace>\n </mrow>\n </msup>\n </mrow>\n <annotation>${{\\umu}}{{{\\mathrm{m}}}^{2\\ }}$</annotation>\n </semantics></math>/ps), <math>\n <semantics>\n <msub>\n <mi>P</mi>\n <mn>0</mn>\n </msub>\n <annotation>${{{\\mathrm{P}}}_0}$</annotation>\n </semantics></math> is the scaling parameter equal to 445 <math>\n <semantics>\n <mrow>\n <msub>\n <mi>γ</mi>\n <mrow>\n <mi>C</mi>\n <mspace></mspace>\n </mrow>\n </msub>\n <msub>\n <mi>γ</mi>\n <mrow>\n <mi>R</mi>\n <mspace></mspace>\n </mrow>\n </msub>\n <mo>/</mo>\n <mi>R</mi>\n </mrow>\n <annotation>${{{{\\gamma}}}_{{\\mathrm{C\\ }}}}{{{{\\gamma}}}_{{\\mathrm{R\\ }}}}/{\\mathrm{R}}$</annotation>\n </semantics></math>.","PeriodicalId":204,"journal":{"name":"Laser & Photonics Reviews","volume":"19 1","pages":""},"PeriodicalIF":9.8000,"publicationDate":"2024-12-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/lpor.202401760","citationCount":"0","resultStr":"{\"title\":\"Correction to “Leaky-Integrate-and-Fire Mechanism in Exciton-Polariton Condensates for Photonic Spiking Neurons”\",\"authors\":\"\",\"doi\":\"10.1002/lpor.202401760\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"K. Tyszka, M. Furman, R. Mirek, M. Król, A. Opala, B. Seredyński, J. Suffczyński, W. Pacuski, M. Matuszewski, J. Szczytko, B. Piętka, Leaky Integrate-and-Fire Mechanism in Exciton–Polariton Condensates for Photonic Spiking Neurons. Laser Photonics Rev 2022, 17, 2100660. https://doi.org/10.1002/lpor.202100660In this article, an error was identified in the caption and panel numbering of Figure 5. Panels (d) and (e) were inadvertently switched, and two of the panel references were omitted from the caption.The revised version of Figure 5, along with its caption, is provided below.Figure 5 (a) Dependence of the delay <math>\\n <semantics>\\n <mrow>\\n <mi>Δ</mi>\\n <mi>t</mi>\\n </mrow>\\n <annotation>$\\\\Delta {\\\\mathrm{t}}$</annotation>\\n </semantics></math> between the peak of the pumping pulse P(t) and the peak of the condensate emission <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>n</mi>\\n <mi>C</mi>\\n </msub>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation>${{{\\\\mathrm{n}}}_{\\\\mathrm{C}}}( {\\\\mathrm{t}} )$</annotation>\\n </semantics></math> on the peak pumping power P. (b, c) Evolution of condensate density <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>n</mi>\\n <mi>C</mi>\\n </msub>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation>${{{\\\\mathrm{n}}}_{\\\\mathrm{C}}}( {\\\\mathrm{t}} )$</annotation>\\n </semantics></math> and the inactive reservoir density <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>n</mi>\\n <mi>i</mi>\\n </msub>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation>${{{\\\\mathrm{n}}}_{\\\\mathrm{i}}}( {\\\\mathrm{t}} )$</annotation>\\n </semantics></math> for the two pumping powers marked in (a). (d, e) The corresponding evolution of the active reservoir density <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>n</mi>\\n <mi>R</mi>\\n </msub>\\n <mrow>\\n <mo>(</mo>\\n <mi>t</mi>\\n <mo>)</mo>\\n </mrow>\\n </mrow>\\n <annotation>${{{\\\\mathrm{n}}}_{\\\\mathrm{R}}}( {\\\\mathrm{t}} )$</annotation>\\n </semantics></math>. Parameters: <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>γ</mi>\\n <mi>C</mi>\\n </msub>\\n <mo>=</mo>\\n <mn>1</mn>\\n <mo>/</mo>\\n <mn>12</mn>\\n </mrow>\\n <annotation>${{{{\\\\gamma}}}_{\\\\mathrm{C}}} = 1/12$</annotation>\\n </semantics></math> (1/ps), <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>γ</mi>\\n <mi>R</mi>\\n </msub>\\n <mo>=</mo>\\n <mn>1</mn>\\n <mo>/</mo>\\n <mn>200</mn>\\n </mrow>\\n <annotation>${{{{\\\\gamma}}}_{\\\\mathrm{R}}} = 1/200$</annotation>\\n </semantics></math> (1/ps), <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>γ</mi>\\n <mi>I</mi>\\n </msub>\\n <mo>=</mo>\\n <mn>1</mn>\\n <mo>/</mo>\\n <mn>1000</mn>\\n </mrow>\\n <annotation>${{{{\\\\gamma}}}_{\\\\mathrm{I}}} = 1/1000$</annotation>\\n </semantics></math> (1/ps), <math>\\n <semantics>\\n <mrow>\\n <mi>R</mi>\\n <mo>=</mo>\\n <mn>6</mn>\\n <mo>×</mo>\\n <msup>\\n <mn>10</mn>\\n <mrow>\\n <mo>−</mo>\\n <mn>4</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>${\\\\mathrm{R}} = 6 \\\\times {{10}^{ - 4}}$</annotation>\\n </semantics></math>(<math>\\n <semantics>\\n <mrow>\\n <mi>μ</mi>\\n <msup>\\n <mi>m</mi>\\n <mrow>\\n <mn>2</mn>\\n <mspace></mspace>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>${{\\\\umu}}{{{\\\\mathrm{m}}}^{2\\\\ }}$</annotation>\\n </semantics></math>/ps), <math>\\n <semantics>\\n <mrow>\\n <mi>κ</mi>\\n <mo>=</mo>\\n <mn>5</mn>\\n <mo>×</mo>\\n <msup>\\n <mn>10</mn>\\n <mrow>\\n <mo>−</mo>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>${{\\\\kappa}} = 5 \\\\times {{10}^{ - 2}}$</annotation>\\n </semantics></math>(<math>\\n <semantics>\\n <mrow>\\n <mi>μ</mi>\\n <msup>\\n <mi>m</mi>\\n <mrow>\\n <mn>2</mn>\\n <mspace></mspace>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>${{\\\\umu}}{{{\\\\mathrm{m}}}^{2\\\\ }}$</annotation>\\n </semantics></math>/ps), <math>\\n <semantics>\\n <msub>\\n <mi>P</mi>\\n <mn>0</mn>\\n </msub>\\n <annotation>${{{\\\\mathrm{P}}}_0}$</annotation>\\n </semantics></math> is the scaling parameter equal to 445 <math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>γ</mi>\\n <mrow>\\n <mi>C</mi>\\n <mspace></mspace>\\n </mrow>\\n </msub>\\n <msub>\\n <mi>γ</mi>\\n <mrow>\\n <mi>R</mi>\\n <mspace></mspace>\\n </mrow>\\n </msub>\\n <mo>/</mo>\\n <mi>R</mi>\\n </mrow>\\n <annotation>${{{{\\\\gamma}}}_{{\\\\mathrm{C\\\\ }}}}{{{{\\\\gamma}}}_{{\\\\mathrm{R\\\\ }}}}/{\\\\mathrm{R}}$</annotation>\\n </semantics></math>.\",\"PeriodicalId\":204,\"journal\":{\"name\":\"Laser & Photonics Reviews\",\"volume\":\"19 1\",\"pages\":\"\"},\"PeriodicalIF\":9.8000,\"publicationDate\":\"2024-12-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1002/lpor.202401760\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Laser & Photonics Reviews\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1002/lpor.202401760\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Laser & Photonics Reviews","FirstCategoryId":"101","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/lpor.202401760","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"OPTICS","Score":null,"Total":0}

引用次数: 0

摘要

K. Tyszka， M. Furman， R. Mirek， M. Król， A. Opala， B. Seredyński， J. Suffczyński， W. Pacuski， M. Matuszewski， J. Szczytko， B. Piętka，光子脉冲神经元激子-极化凝聚体的泄漏积分-燃烧机制。激光光子学，2022,17,2100660。在本文https://doi.org/10.1002/lpor.202100660In中，在图5的标题和面板编号中发现了一个错误。面板(d)和(e)被无意中切换，并且在标题中省略了两个面板参考文献。图5的修订版本及其标题如下所示。图5 (a)泵送脉冲峰值P(t)与凝析油排放峰值nC (t) ${{{\mathrm{n}}}_{\mathrm{C}}}( {\mathrm{t}} )$之间的延迟Δ¹$\Delta {\mathrm{t}}$与峰值泵送功率P的关系（b, c） (a)中标注的两种泵送功率下凝析油密度nC (t) ${{{\mathrm{n}}}_{\mathrm{C}}}( {\mathrm{t}} )$与非活动油藏密度ni (t) ${{{\mathrm{n}}}_{\mathrm{i}}}( {\mathrm{t}} )$的演化关系。（d, e）活动油藏密度nR (t) ${{{\mathrm{n}}}_{\mathrm{R}}}( {\mathrm{t}} )$的相应演化关系。参数：γC=1/12 ${{{{\gamma}}}_{\mathrm{C}}} = 1/12$ (1/ps), γR=1/200 ${{{{\gamma}}}_{\mathrm{R}}} = 1/200$ (1/ps), γI=1/1000 ${{{{\gamma}}}_{\mathrm{I}}} = 1/1000$ (1/ps)， R=6×10−4 ${\mathrm{R}} = 6 \times {{10}^{ - 4}}$ (μ减去m2 ${{\umu}}{{{\mathrm{m}}}^{2\ }}$ /ps), κ=5×10−2 ${{\kappa}} = 5 \times {{10}^{ - 2}}$ (μ减去m2 ${{\umu}}{{{\mathrm{m}}}^{2\ }}$ /ps), P0 ${{{\mathrm{P}}}_0}$是缩放参数等于445 γC减去γR/R ${{{{\gamma}}}_{{\mathrm{C\ }}}}{{{{\gamma}}}_{{\mathrm{R\ }}}}/{\mathrm{R}}$。

本文章由计算机程序翻译，如有差异，请以英文原文为准。

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Correction to “Leaky-Integrate-and-Fire Mechanism in Exciton-Polariton Condensates for Photonic Spiking Neurons”

K. Tyszka, M. Furman, R. Mirek, M. Król, A. Opala, B. Seredyński, J. Suffczyński, W. Pacuski, M. Matuszewski, J. Szczytko, B. Piętka, Leaky Integrate-and-Fire Mechanism in Exciton–Polariton Condensates for Photonic Spiking Neurons. Laser Photonics Rev 2022, 17, 2100660. https://doi.org/10.1002/lpor.202100660

In this article, an error was identified in the caption and panel numbering of Figure 5. Panels (d) and (e) were inadvertently switched, and two of the panel references were omitted from the caption.

The revised version of Figure 5, along with its caption, is provided below.

Figure 5 (a) Dependence of the delay $Δ t$ between the peak of the pumping pulse P(t) and the peak of the condensate emission $n_{C} (t)$ on the peak pumping power P. (b, c) Evolution of condensate density $n_{C} (t)$ and the inactive reservoir density $n_{i} (t)$ for the two pumping powers marked in (a). (d, e) The corresponding evolution of the active reservoir density $n_{R} (t)$ . Parameters: $γ_{C} = 1 / 12$ (1/ps), $γ_{R} = 1 / 200$ (1/ps), $γ_{I} = 1 / 1000$ (1/ps), $R = 6 \times 10^{- 4}$ ( $μ m^{2}$ /ps), $κ = 5 \times 10^{- 2}$ ( $μ m^{2}$ /ps), $P_{0}$ is the scaling parameter equal to 445 $γ_{C} γ_{R} / R$ .

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来源期刊

Laser & Photonics Reviews 物理-光学

CiteScore

14.20

自引率

5.50%

发文量

314

审稿时长

2 months

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